project_folder = "/Volumes/GoogleDrive/My Drive/Melbourne/UNIMELB/Research/Complexity Project/ICx3_new/Code/behavAnalysis/ICx3_supp/"
code_folder = paste0(project_folder, "Code/")
data_folder = paste0(project_folder, "Data/")

setwd(code_folder)
knitr::opts_knit$set(root.dir = code_folder)

#Import functions
source(file.path(code_folder,"DescriptiveFunctions.R"))

# Participant Data
folderModels = "/Volumes/GoogleDrive/My Drive/Melbourne/UNIMELB/Research/Complexity Project/ICx3_new/Code/behavAnalysis/Output/"

folderOut_figures = paste0(project_folder,"Output/Figures")
folderOut_tables = paste0(project_folder,"Output/Tables")
## Setting up the basics
library(ggplot2)
library(knitr)
library(dplyr)
library(ggsignif)
library(pander)
library(plotly)
library(reshape2)
library(Hmisc)
library(readr)
library(brms)
library(parallel)
library(sjstats)
library(bayesplot)
library(bmlm)
library(DiagrammeR)
library(tidyr)

#From easystats:
library(parameters)
library(see)
library(bayestestR)
library(performance)
library(forcats)
library(ggpol)
# brms Input

chains_brms = 4
cores_brms = min(chains_brms,detectCores())
seed_brms = 111
iters_high = 4000
# Functions
save_summarise_model = function(model, modelName){
  if (modelName %in% names(allModels)){
    warning("Model Name already exists!")
    model = allModels[[modelName]]
  } else {
    allModels[[modelName]]<<- model
  }
 
    table = model_parameters(model, 
                              ci_method = "HDI",ci=0.95,test = c("hdi","pd"))
    
    table2 = performance::model_performance(model,metrics="common")

    plo = plot(hdi(model, ci = c(0.95)), data = model)+
          ggtitle("Posterior distributions",
                  "with medians and 95% quantile-based-intervals") +
          theme(plot.title = element_text(hjust = 0.5),
                plot.subtitle = element_text(hjust = 0.5))
  
    print(as_tibble(table))
    print(as_tibble(table2))
    print(plo)
    
    allModels[[modelName]]<<- model
}
# Use current models or rerun everything Comment one option

# allModels := list of all the regressions that are run 


## Option1: Use current saved models

# Import estimated models
allModels = read_rds(file.path(folderModels,"ICx3_models_KS.RData"))

# Don't run brms models
brm2 =  function(...){
  return(FALSE)
}

# ## Option2: Rerun everything from scratch
# 
# allModels=vector("list", length=0)
# 
# brm2 =  function(...){
#   return(brm(...))
# }

1 Knapsack decision problem (KP)

2 Accuracy

Read Clean Data to file


dataTrial_KS= read_csv(file.path(data_folder,"KSDec_clean.csv"),
                       col_types = cols(w = col_character(),
                                        v = col_character()))


dataTrial_KS$region = case_when(
  dataTrial_KS$type %in% c(1,2,3,4) ~ "Phase Transition",
  dataTrial_KS$type %in% c(6) ~ "Underconstrained",
  dataTrial_KS$type %in% c(5) ~ "Overconstrained"
)

2.1 Satisfiability

dataInput=dataTrial_KS

logitRandomIntercept = brm2(correct ~ sol + (1|pID),
                           family=bernoulli(link="logit"),
                           data=dataInput,
                           chains=chains_brms,
                           cores = cores_brms,
                           seed=seed_brms,
                           refresh = 0,
                           save_all_pars = TRUE)

tableName='ks_acc_sat1'
save_summarise_model(logitRandomIntercept, tableName)
Model Name already exists!

2.2 Number of witnesses

2.2.1 With TCC

dataInput=dataTrial_KS

dataInput = dataInput %>% filter(sol==1)

dataInput$nSolutions_log =log(dataInput$nSolutions)
logitRandomIntercept = brm2(correct ~ nSolutions + phaseT + phaseT:nSolutions + (1|pID),
                           family=bernoulli(link="logit"),
                           data=dataInput,
                           chains=chains_brms,
                           cores = cores_brms,
                           seed=seed_brms,
                           refresh = 0,
                           save_all_pars = TRUE)

tableName='ks_acc_ns1'
save_summarise_model(allModels[['ks_acc_ns1']], tableName)
Model Name already exists!

model = allModels[['ks_acc_ns1']]
plot(marginal_effects(model), plot = TRUE, ask = FALSE)
Method 'marginal_effects' is deprecated. Please use 'conditional_effects' instead.

2.2.2 With TCC (no interaction)

dataInput=dataTrial_KS

dataInput = dataInput %>% filter(sol==1)

logitRandomIntercept = brm2(correct ~ nSolutions + phaseT +  (1|pID),
                           family=bernoulli(link="logit"),
                           data=dataInput,
                           chains=chains_brms,
                           cores = cores_brms,
                           seed=seed_brms,
                           refresh = 0,
                           save_all_pars = TRUE)

tableName='ks_acc_ns2'
save_summarise_model(allModels[['ks_acc_ns2']], tableName)
Model Name already exists!

Marginal Effects

#marginal_effects(logitRandomIntercept, ask=FALSE)
plot(marginal_effects(allModels[['ks_acc_ns2']]), plot = TRUE, ask = FALSE)
Method 'marginal_effects' is deprecated. Please use 'conditional_effects' instead.

2.2.3 Alone

dataInput=dataTrial_KS

dataInput = dataInput %>% filter(sol==1)

logitRandomIntercept = brm2(correct ~ nSolutions +  (1|pID),
                           family=bernoulli(link="logit"),
                           data=dataInput,
                           chains=chains_brms,
                           cores = cores_brms,
                           seed=seed_brms,
                           refresh = 0,
                           save_all_pars = TRUE)

# m3 = logitRandomIntercept
tableName='ks_acc_ns3'
save_summarise_model(allModels[['ks_acc_ns3']], tableName)
Model Name already exists!

2.2.3.1 Plot

dataInput=dataTrial_KS

dataInput = dataInput %>% filter(sol==1)

model_ICexpost = allModels[['ks_acc_ns3']]

mean_accuracy = dataInput %>% group_by(id,phaseT,sol,nSolutions,ICexpost) %>% 
  summarise(accuracy = mean(correct))
`summarise()` regrouping output by 'id', 'phaseT', 'sol', 'nSolutions' (override with `.groups` argument)
pp  = plot(conditional_effects(model_ICexpost), plot = TRUE, ask = FALSE)


pp$nSolutions + 
  geom_point(data=mean_accuracy,aes(x = nSolutions, y = accuracy, col=as.factor(phaseT)),inherit.aes = FALSE)+
  theme_minimal()

# Improving the plot
size_big = 20
size_small = 16
size_ss = 10
size_xs = 7

pp_plot = pp$nSolutions
pp_plot$layers[[1]]$geom_params$se = FALSE
pp_plot$layers[[1]]$aes_params$colour="#577590"

pp_plot$layers <- c(geom_point(data=mean_accuracy,
                               aes(x = nSolutions, y = accuracy, col=as.factor(sol),
                                   shape=as.factor(phaseT), size=2.5), inherit.aes = FALSE),
                         pp_plot$layers)


plo = pp_plot +
  xlab("Number of solution witnesses")+#expression(IC[expost]))+
  ylab("Human Performance")+
  scale_shape_manual(name="",values = c(17,16)) +
  scale_color_manual(name="",values = c("1"="#90BE6D","0"="#F94144"))+# c( "#FC4E07","#E7B800"))+
  theme_classic()+
  theme(axis.title = element_text(size= size_big),
       axis.text=element_text(size=size_small),
       legend.position = "none")+
  guides(shape = guide_legend(override.aes = list(size = 3)))+
  scale_x_continuous(breaks = c(1,5,9,13))+
  ylim(0.2,1)

plo
ggsave(paste0(folderOut_figures,"/Nwit_KS_acc.pdf"),plo,width = 6,height =6,units="in")

2.3 ICexpost

2.3.1 All instances

dataInput = dataTrial_KS
model_ICexpost = brm2(correct ~ ICexpost + (1|pID),
                           family=bernoulli(link="logit"),
                           data=dataInput,
                           chains=chains_brms,
                           cores = cores_brms,
                           seed=seed_brms,
                           refresh = 0)

tableName='ks_acc_icexpost1'
save_summarise_model(allModels[['ks_acc_icexpost1']], tableName)
Model Name already exists!

2.3.1.0.1 Model Fit
#st05
dataInput = dataTrial_KS

model_ICexpost = allModels[['ks_acc_icexpost1']]

# Make predictions excluding random effects (pID)
predictions = predict(model_ICexpost, dataInput, re_formula = NA)

# Estimating the significance of the fit. This is done considering the probability estimation rather than the binary classification.

#Performs the Hosmer-Lemeshow goodness of fit test
logistic_significance = generalhoslem::logitgof(dataInput$correct, 
                                                predictions[,1], g = 10, ord = FALSE)
logistic_significance

    Hosmer and Lemeshow test (binary model)

data:  dataInput$correct, predictions[, 1]
X-squared = 60.184, df = 8, p-value = 4.288e-10
# Finds R2 using binary outcomes
# https://stackoverflow.com/questions/40901445/function-to-calculate-r2-r-squared-in-r
#predictions = predict(model_ICexpost,dataInput, re_formula = NA)
r_2_binary = cor(dataInput$correct, predictions[,1])^2
r_2_binary
[1] 0.1171649
# Finds R2 using mean accuracies per instance
predictions2 = predict(model_ICexpost,mean_accuracy, re_formula = NA)
r_2_probabilities = cor(mean_accuracy$accuracy, predictions2[,1])^2
r_2_probabilities
[1] 0.466316

2.3.1.1 Plot

dataInput = dataTrial_KS
model_ICexpost = allModels[['ks_acc_icexpost1']]

mean_accuracy = dataInput %>% group_by(instanceNumber,phaseT,sol,ICexpost) %>% 
  summarise(accuracy = mean(correct))
`summarise()` regrouping output by 'instanceNumber', 'phaseT', 'sol' (override with `.groups` argument)
pp  = plot(conditional_effects(model_ICexpost), plot = TRUE, ask = FALSE)


pp$ICexpost + 
  geom_point(data=mean_accuracy,aes(x = ICexpost, y = accuracy, col=as.factor(phaseT)),inherit.aes = FALSE)+
  theme_minimal()

# Improving the plot
size_big = 20
size_small = 16
size_ss = 10
size_xs = 7

pp_plot = pp$ICexpost
pp_plot$layers[[1]]$geom_params$se = FALSE
pp_plot$layers[[1]]$aes_params$colour="#577590"

pp_plot$layers <- c(geom_point(data=mean_accuracy,
                               aes(x = ICexpost, y = accuracy, col=as.factor(sol),
                                   shape=as.factor(phaseT), size=2.5), inherit.aes = FALSE),
                         pp_plot$layers)


plo = pp_plot +
# geom_point(data=mean_accuracy,aes(x = ICexpost, y = correct, col=as.factor(sol),shape=as.factor(phaseT), size=2.5),inherit.aes = FALSE)+
  xlab("Instance Complexity (IC)")+#expression(IC[expost]))+
  ylab("Human Performance")+
  scale_shape_manual(name="",values = c(17,16)) +
  scale_color_manual(name="",values = c("1"="#90BE6D","0"="#F94144"))+# c( "#FC4E07","#E7B800"))+
  # scale_shape_manual(name="IC",values = c(2, 8))+
  # scale_color_manual(name="Solution",values = c("red", "blue"))+
  theme_classic()+
  theme(axis.title = element_text(size= size_big),
       axis.text=element_text(size=size_small),
       legend.position = "none")+
  guides(shape = guide_legend(override.aes = list(size = 3)))+
  ylim(0.2,1)

plo
ggsave(paste0(folderOut_figures,"/IC_KS_acc.pdf"),plo,width = 6,height =6,units="in")

2.3.2 Unsatisfiable instances

dataInput = dataTrial_KS
dataInput = dataInput %>% filter(sol==0)
model_ICexpost = brm2(correct ~ ICexpost + (1|pID),
                           family=bernoulli(link="logit"),
                           data=dataInput,
                           chains=chains_brms,
                           cores = cores_brms,
                           seed=seed_brms,
                           refresh = 0)

tableName='ks_acc_icexpost2'
save_summarise_model(allModels[['ks_acc_icexpost2']], tableName)
Model Name already exists!

2.4 Plot TCC


dataInput = dataTrial_KS
dataInput = dataInput %>% 
  mutate(region = fct_relevel(region,
                              "Underconstrained", "Phase Transition", "Overconstrained"))

dataInput2 = dataInput %>% group_by(instanceNumber,region) %>%
  summarise(accuracy=mean(correct))
`summarise()` regrouping output by 'instanceNumber' (override with `.groups` argument)
size_big = 20
size_small = 16
size_ss = 10
size_xs = 7

plo = ggplot(dataInput2,aes(x=region,y=accuracy,fill=region))+
  geom_boxjitter(aes(fill=region),jitter.color = NA,jitter.shape = 21)+
  theme(panel.grid.major = element_blank(), panel.grid.minor = element_blank(),plot.title = element_text(hjust = 0.5))+
  scale_fill_manual(name  ="Region",
                    breaks=c("Underconstrained", "Phase Transition", "Overconstrained"),
                    labels=c("Underconstrained", "Phase Transition", "Overconstrained"),
                    values=c(rgb(249,199,79, max=255),
                             rgb(205,54,56, max=255),
                             rgb(249,199,79, max=255)))+
  geom_signif(annotations = c("***","***"),
             y_position=c(1.05,1.05),xmin=c(1.05,2.1),xmax=c(1.9,2.95))+
  xlab("Typical Case Complexity (TCC)")+
  ylab("Human Performance")+
  theme_classic()+
  theme(axis.title = element_text(size= size_big),
       axis.text=element_text(size=size_small),
       legend.position = "none")+
  guides(shape = guide_legend(override.aes = list(size = 3)))


plo
ggsave(paste0(folderOut_figures,"/TCC_KS_acc.pdf"),plo,width = 6,height =6,units="in")

#brewer
dataInput = dataTrial_KS
dataInput = dataInput %>%
  mutate(region = fct_relevel(region,
                              "Underconstrained", "Phase Transition", "Overconstrained"))%>%
  mutate(sol= as.factor(sol)) %>%
  mutate(sol = fct_relevel(sol,"1", "0"))

dataInput2 = dataInput %>%
  group_by(instanceNumber,region,sol) %>%
  summarise(accuracy=mean(correct))
`summarise()` regrouping output by 'instanceNumber', 'region' (override with `.groups` argument)

plo = ggplot(dataInput2,aes(x=region,y=accuracy,fill=sol))+
  # geom_boxjitter(aes(fill=region),jitter.color = NA,jitter.shape = 21)+
  geom_boxjitter(jitter.color = NA,jitter.shape = 21,
                 jitter.params = list(height=0,seed=10),
                 outlier.shape= NA)+
                 #,outlier.shape = 4, outlier.size=0.9)+
  theme(panel.grid.major = element_blank(), panel.grid.minor = element_blank(),
        plot.title = element_text(hjust = 0.5))+
  scale_fill_manual(name  ="Region",
                    breaks=c("1","0"),
                    labels=c("Satisfiable","Unsatisfiable"),
                    values=c("#90BE6D","#F94144"))+
  xlab("Typical Case Complexity (TCC)")+
  ylab("Human Performance")+
  theme_classic()+
  theme(axis.title = element_text(size= size_big),
       axis.text=element_text(size=size_small),
       legend.position = "none")+
  guides(shape = guide_legend(override.aes = list(size = 3)))+
  ylim(0.2,1)

plo
ggsave(paste0(folderOut_figures,"/TCC_KS_acc1.pdf"),plo,width = 7,height =6,units="in")

3 Save Models

# saveRDS(allModels,file.path(folderOut,"ICx3_models_KS.RData"))
---
title: "Behavioural results for the knapsack task"
author: "J. Pablo Franco"
date: "`r format(Sys.time(), '%d %B, %Y')`"
output: 
  html_notebook: 
    code_folding: hide
    number_sections: yes
    theme: united
    toc: yes
    toc_float: yes
---

```{r doc_setup, include=FALSE}
knitr::opts_chunk$set(echo = TRUE)
```

```{=html}
<style>

table, td, th {
  border: none;
  padding-left: 1em;
  padding-right: 1em;
  min-width: 50%;
  margin-left: auto;
  margin-right: auto;
  margin-top: 1em;
  margin-bottom: 1em;
}

</style>
```

```{r folder_management}

project_folder = "/Volumes/GoogleDrive/My Drive/Melbourne/UNIMELB/Research/Complexity Project/ICx3_new/Code/behavAnalysis/ICx3_supp/"
code_folder = paste0(project_folder, "Code/")
data_folder = paste0(project_folder, "Data/")

setwd(code_folder)
knitr::opts_knit$set(root.dir = code_folder)

#Import functions
source(file.path(code_folder,"DescriptiveFunctions.R"))

# Participant Data
folderModels = "/Volumes/GoogleDrive/My Drive/Melbourne/UNIMELB/Research/Complexity Project/ICx3_new/Code/behavAnalysis/Output/"

folderOut_figures = paste0(project_folder,"Output/Figures")
folderOut_tables = paste0(project_folder,"Output/Tables")
```

```{r setup, collapse=TRUE}
## Setting up the basics
library(ggplot2)
library(knitr)
library(dplyr)
library(ggsignif)
library(pander)
library(plotly)
library(reshape2)
library(Hmisc)
library(readr)
library(brms)
library(parallel)
library(sjstats)
library(bayesplot)
library(bmlm)
library(DiagrammeR)
library(tidyr)

#From easystats:
library(parameters)
library(see)
library(bayestestR)
library(performance)
library(forcats)
library(ggpol)

```

```{r}
# brms Input

chains_brms = 4
cores_brms = min(chains_brms,detectCores())
seed_brms = 111
iters_high = 4000

```

```{r}
# Functions
save_summarise_model = function(model, modelName){
  if (modelName %in% names(allModels)){
    warning("Model Name already exists!")
    model = allModels[[modelName]]
  } else {
    allModels[[modelName]]<<- model
  }
 
    table = model_parameters(model, 
                              ci_method = "HDI",ci=0.95,test = c("hdi","pd"))
    
    table2 = performance::model_performance(model,metrics="common")

    plo = plot(hdi(model, ci = c(0.95)), data = model)+
          ggtitle("Posterior distributions",
                  "with medians and 95% quantile-based-intervals") +
          theme(plot.title = element_text(hjust = 0.5),
                plot.subtitle = element_text(hjust = 0.5))
  
    print(as_tibble(table))
    print(as_tibble(table2))
    print(plo)
    
    allModels[[modelName]]<<- model
}

```

```{r}
# Use current models or rerun everything Comment one option

# allModels := list of all the regressions that are run 


## Option1: Use current saved models

# Import estimated models
allModels = read_rds(file.path(folderModels,"ICx3_models_KS.RData"))

# Don't run brms models
brm2 =  function(...){
  return(FALSE)
}

# ## Option2: Rerun everything from scratch
# 
# allModels=vector("list", length=0)
# 
# brm2 =  function(...){
#   return(brm(...))
# }


```

# Knapsack decision problem (KP)

# Accuracy 

Read Clean Data to file

```{r}

dataTrial_KS= read_csv(file.path(data_folder,"KSDec_clean.csv"),
                       col_types = cols(w = col_character(),
                                        v = col_character()))


dataTrial_KS$region = case_when(
  dataTrial_KS$type %in% c(1,2,3,4) ~ "Phase Transition",
  dataTrial_KS$type %in% c(6) ~ "Underconstrained",
  dataTrial_KS$type %in% c(5) ~ "Overconstrained"
)

```

## Satisfiability

```{r}
dataInput=dataTrial_KS

logitRandomIntercept = brm2(correct ~ sol + (1|pID),
                           family=bernoulli(link="logit"),
                           data=dataInput,
                           chains=chains_brms,
                           cores = cores_brms,
                           seed=seed_brms,
                           refresh = 0,
                           save_all_pars = TRUE)

tableName='ks_acc_sat1'
save_summarise_model(logitRandomIntercept, tableName)
```

## Number of witnesses 

### With TCC

```{r}
dataInput=dataTrial_KS

dataInput = dataInput %>% filter(sol==1)

dataInput$nSolutions_log =log(dataInput$nSolutions)
logitRandomIntercept = brm2(correct ~ nSolutions + phaseT + phaseT:nSolutions + (1|pID),
                           family=bernoulli(link="logit"),
                           data=dataInput,
                           chains=chains_brms,
                           cores = cores_brms,
                           seed=seed_brms,
                           refresh = 0,
                           save_all_pars = TRUE)

tableName='ks_acc_ns1'
save_summarise_model(allModels[['ks_acc_ns1']], tableName)
```

```{r}
model = allModels[['ks_acc_ns1']]
plot(marginal_effects(model), plot = TRUE, ask = FALSE)
```

### With TCC (no interaction)

```{r}
dataInput=dataTrial_KS

dataInput = dataInput %>% filter(sol==1)

logitRandomIntercept = brm2(correct ~ nSolutions + phaseT +  (1|pID),
                           family=bernoulli(link="logit"),
                           data=dataInput,
                           chains=chains_brms,
                           cores = cores_brms,
                           seed=seed_brms,
                           refresh = 0,
                           save_all_pars = TRUE)

tableName='ks_acc_ns2'
save_summarise_model(allModels[['ks_acc_ns2']], tableName)
```

Marginal Effects

```{r}
#marginal_effects(logitRandomIntercept, ask=FALSE)
plot(marginal_effects(allModels[['ks_acc_ns2']]), plot = TRUE, ask = FALSE)
```

### Alone

```{r}
dataInput=dataTrial_KS

dataInput = dataInput %>% filter(sol==1)

logitRandomIntercept = brm2(correct ~ nSolutions +  (1|pID),
                           family=bernoulli(link="logit"),
                           data=dataInput,
                           chains=chains_brms,
                           cores = cores_brms,
                           seed=seed_brms,
                           refresh = 0,
                           save_all_pars = TRUE)

# m3 = logitRandomIntercept
tableName='ks_acc_ns3'
save_summarise_model(allModels[['ks_acc_ns3']], tableName)

```

#### Plot

```{r}
dataInput=dataTrial_KS

dataInput = dataInput %>% filter(sol==1)

model_ICexpost = allModels[['ks_acc_ns3']]

mean_accuracy = dataInput %>% group_by(id,phaseT,sol,nSolutions,ICexpost) %>% 
  summarise(accuracy = mean(correct))

pp  = plot(conditional_effects(model_ICexpost), plot = TRUE, ask = FALSE)

pp$nSolutions + 
  geom_point(data=mean_accuracy,aes(x = nSolutions, y = accuracy, col=as.factor(phaseT)),inherit.aes = FALSE)+
  theme_minimal()
```

```{r}
# Improving the plot
size_big = 20
size_small = 16
size_ss = 10
size_xs = 7

pp_plot = pp$nSolutions
pp_plot$layers[[1]]$geom_params$se = FALSE
pp_plot$layers[[1]]$aes_params$colour="#577590"

pp_plot$layers <- c(geom_point(data=mean_accuracy,
                               aes(x = nSolutions, y = accuracy, col=as.factor(sol),
                                   shape=as.factor(phaseT), size=2.5), inherit.aes = FALSE),
                         pp_plot$layers)


plo = pp_plot +
  xlab("Number of solution witnesses")+#expression(IC[expost]))+
  ylab("Human Performance")+
  scale_shape_manual(name="",values = c(17,16)) +
  scale_color_manual(name="",values = c("1"="#90BE6D","0"="#F94144"))+# c( "#FC4E07","#E7B800"))+
  theme_classic()+
  theme(axis.title = element_text(size= size_big),
       axis.text=element_text(size=size_small),
       legend.position = "none")+
  guides(shape = guide_legend(override.aes = list(size = 3)))+
  scale_x_continuous(breaks = c(1,5,9,13))+
  ylim(0.2,1)

plo
ggsave(paste0(folderOut_figures,"/Nwit_KS_acc.pdf"),plo,width = 6,height =6,units="in")
```

## ICexpost

### All instances

```{r}
dataInput = dataTrial_KS
model_ICexpost = brm2(correct ~ ICexpost + (1|pID),
                           family=bernoulli(link="logit"),
                           data=dataInput,
                           chains=chains_brms,
                           cores = cores_brms,
                           seed=seed_brms,
                           refresh = 0)

tableName='ks_acc_icexpost1'
save_summarise_model(allModels[['ks_acc_icexpost1']], tableName)

```

##### Model Fit

```{r}
#st05
dataInput = dataTrial_KS

model_ICexpost = allModels[['ks_acc_icexpost1']]

# Make predictions excluding random effects (pID)
predictions = predict(model_ICexpost, dataInput, re_formula = NA)

# Estimating the significance of the fit. This is done considering the probability estimation rather than the binary classification.

#Performs the Hosmer-Lemeshow goodness of fit test
logistic_significance = generalhoslem::logitgof(dataInput$correct, 
                                                predictions[,1], g = 10, ord = FALSE)
logistic_significance

# Finds R2 using binary outcomes
# https://stackoverflow.com/questions/40901445/function-to-calculate-r2-r-squared-in-r
#predictions = predict(model_ICexpost,dataInput, re_formula = NA)
r_2_binary = cor(dataInput$correct, predictions[,1])^2
r_2_binary

# Finds R2 using mean accuracies per instance
predictions2 = predict(model_ICexpost,mean_accuracy, re_formula = NA)
r_2_probabilities = cor(mean_accuracy$accuracy, predictions2[,1])^2
r_2_probabilities
```

#### Plot

```{r}
dataInput = dataTrial_KS
model_ICexpost = allModels[['ks_acc_icexpost1']]

mean_accuracy = dataInput %>% group_by(instanceNumber,phaseT,sol,ICexpost) %>% 
  summarise(accuracy = mean(correct))

pp  = plot(conditional_effects(model_ICexpost), plot = TRUE, ask = FALSE)

pp$ICexpost + 
  geom_point(data=mean_accuracy,aes(x = ICexpost, y = accuracy, col=as.factor(phaseT)),inherit.aes = FALSE)+
  theme_minimal()
```

```{r}
# Improving the plot
size_big = 20
size_small = 16
size_ss = 10
size_xs = 7

pp_plot = pp$ICexpost
pp_plot$layers[[1]]$geom_params$se = FALSE
pp_plot$layers[[1]]$aes_params$colour="#577590"

pp_plot$layers <- c(geom_point(data=mean_accuracy,
                               aes(x = ICexpost, y = accuracy, col=as.factor(sol),
                                   shape=as.factor(phaseT), size=2.5), inherit.aes = FALSE),
                         pp_plot$layers)


plo = pp_plot +
# geom_point(data=mean_accuracy,aes(x = ICexpost, y = correct, col=as.factor(sol),shape=as.factor(phaseT), size=2.5),inherit.aes = FALSE)+
  xlab("Instance Complexity (IC)")+#expression(IC[expost]))+
  ylab("Human Performance")+
  scale_shape_manual(name="",values = c(17,16)) +
  scale_color_manual(name="",values = c("1"="#90BE6D","0"="#F94144"))+# c( "#FC4E07","#E7B800"))+
  # scale_shape_manual(name="IC",values = c(2, 8))+
  # scale_color_manual(name="Solution",values = c("red", "blue"))+
  theme_classic()+
  theme(axis.title = element_text(size= size_big),
       axis.text=element_text(size=size_small),
       legend.position = "none")+
  guides(shape = guide_legend(override.aes = list(size = 3)))+
  ylim(0.2,1)

plo
ggsave(paste0(folderOut_figures,"/IC_KS_acc.pdf"),plo,width = 6,height =6,units="in")
```

### Unsatisfiable instances

```{r}
dataInput = dataTrial_KS
dataInput = dataInput %>% filter(sol==0)
model_ICexpost = brm2(correct ~ ICexpost + (1|pID),
                           family=bernoulli(link="logit"),
                           data=dataInput,
                           chains=chains_brms,
                           cores = cores_brms,
                           seed=seed_brms,
                           refresh = 0)

tableName='ks_acc_icexpost2'
save_summarise_model(allModels[['ks_acc_icexpost2']], tableName)

```

## Plot TCC

```{r}

dataInput = dataTrial_KS
dataInput = dataInput %>% 
  mutate(region = fct_relevel(region,
                              "Underconstrained", "Phase Transition", "Overconstrained"))

dataInput2 = dataInput %>% group_by(instanceNumber,region) %>%
  summarise(accuracy=mean(correct))

```

```{r}
size_big = 20
size_small = 16
size_ss = 10
size_xs = 7

plo = ggplot(dataInput2,aes(x=region,y=accuracy,fill=region))+
  geom_boxjitter(aes(fill=region),jitter.color = NA,jitter.shape = 21)+
  theme(panel.grid.major = element_blank(), panel.grid.minor = element_blank(),plot.title = element_text(hjust = 0.5))+
  scale_fill_manual(name  ="Region",
                    breaks=c("Underconstrained", "Phase Transition", "Overconstrained"),
                    labels=c("Underconstrained", "Phase Transition", "Overconstrained"),
                    values=c(rgb(249,199,79, max=255),
                             rgb(205,54,56, max=255),
                             rgb(249,199,79, max=255)))+
  geom_signif(annotations = c("***","***"),
             y_position=c(1.05,1.05),xmin=c(1.05,2.1),xmax=c(1.9,2.95))+
  xlab("Typical Case Complexity (TCC)")+
  ylab("Human Performance")+
  theme_classic()+
  theme(axis.title = element_text(size= size_big),
       axis.text=element_text(size=size_small),
       legend.position = "none")+
  guides(shape = guide_legend(override.aes = list(size = 3)))


plo
ggsave(paste0(folderOut_figures,"/TCC_KS_acc.pdf"),plo,width = 6,height =6,units="in")
#brewer
```

```{r}
dataInput = dataTrial_KS
dataInput = dataInput %>%
  mutate(region = fct_relevel(region,
                              "Underconstrained", "Phase Transition", "Overconstrained"))%>%
  mutate(sol= as.factor(sol)) %>%
  mutate(sol = fct_relevel(sol,"1", "0"))

dataInput2 = dataInput %>%
  group_by(instanceNumber,region,sol) %>%
  summarise(accuracy=mean(correct))
```

```{r}

plo = ggplot(dataInput2,aes(x=region,y=accuracy,fill=sol))+
  # geom_boxjitter(aes(fill=region),jitter.color = NA,jitter.shape = 21)+
  geom_boxjitter(jitter.color = NA,jitter.shape = 21,
                 jitter.params = list(height=0,seed=10),
                 outlier.shape= NA)+
                 #,outlier.shape = 4, outlier.size=0.9)+
  theme(panel.grid.major = element_blank(), panel.grid.minor = element_blank(),
        plot.title = element_text(hjust = 0.5))+
  scale_fill_manual(name  ="Region",
                    breaks=c("1","0"),
                    labels=c("Satisfiable","Unsatisfiable"),
                    values=c("#90BE6D","#F94144"))+
  xlab("Typical Case Complexity (TCC)")+
  ylab("Human Performance")+
  theme_classic()+
  theme(axis.title = element_text(size= size_big),
       axis.text=element_text(size=size_small),
       legend.position = "none")+
  guides(shape = guide_legend(override.aes = list(size = 3)))+
  ylim(0.2,1)

plo
ggsave(paste0(folderOut_figures,"/TCC_KS_acc1.pdf"),plo,width = 7,height =6,units="in")
```

# Save Models

```{r}
# saveRDS(allModels,file.path(folderOut,"ICx3_models_KS.RData"))
```

